EP0037413B1 - Strip transmission line tuner circuit - Google Patents
Strip transmission line tuner circuit Download PDFInfo
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- EP0037413B1 EP0037413B1 EP80902089A EP80902089A EP0037413B1 EP 0037413 B1 EP0037413 B1 EP 0037413B1 EP 80902089 A EP80902089 A EP 80902089A EP 80902089 A EP80902089 A EP 80902089A EP 0037413 B1 EP0037413 B1 EP 0037413B1
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- strip
- tuning element
- tuner
- circuit
- tuning
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01P—WAVEGUIDES; RESONATORS, LINES, OR OTHER DEVICES OF THE WAVEGUIDE TYPE
- H01P5/00—Coupling devices of the waveguide type
- H01P5/04—Coupling devices of the waveguide type with variable factor of coupling
Definitions
- the present invention relates to a strip transmission line tuner circuit comprising a pair of tuning elements disposed over a ground plane, each tuning element comprising a first strip of conductive material and a second strip of conductive material, said second strip being equal in length to and positioned in parallel, spaced apart . relationship with the first strip, the second strip of one of said tuning element being connected in series to the first strip of the other tuning element thereby forming an extended conductive strip having the first strip of the said one tuning element and the second strip of the said other tuning element disposed on opposite sides thereof and in longitudinally spaced relationship thereto.
- Such a circuit is disclosed in an article "Synthesis of a Class of Strip-Line Filters" by H. Ozaki et al in IRE Transactions on Circuit Theory, Vol. CT-S No. 2, June 1958, at pages 104-109.
- a transmission line comprises a wide and a narrow conductor mounted in parallel on opposite sides of a substrate.
- a tuning element comprises a first and a second conductor disposed in spaced-apart parallel relationship to each other and normal to the narrow conductor of the transmission line. The ends of the tuning element first and second conductors adjacent the narrow line conductor are coupled thereto, and a coupling means is disposed between and in contact with the first and second conductors.
- the coupling means is longitudinally movable between the first and second adjacent conductors of the tuning element at a distance from the narrow line conductor, and this coupling means forms, in conjunction with the wide conductor of the transmission line directly adjacent the tuning element, and adjustable resonant network.
- stripline filters and directional coupling arrangements are discussed in an article "Coupled-Strip-Transmission-Line Filters and Directional Couplers" by E. M. T. Jones et al in IRE Transactions on Microwave Theory and Techniques, Vol. MTT-4, No. 2, April 1956 at pp. 75-81.
- low-pass, band-pass, all-pass and all-stop basic filter characteristics are obtained from a pair of parallel, spaced-apart, strips either by placing open or short circuits at two of the four available terminals pairs, or by interconnecting two of the terminal pairs.
- the article further describes how desired performance may be achieved by cascading several of the basic filter sections.
- the problem remaining in the prior art is to provide a class of tuners which are capable of being formed directly on the microstrip or strip- line medium so as to be close to the device being tested, thereby to increase the usable frequency range of the tuner, and also which are capable of matching any impedance falling within the Smith chart.
- each tuning element comprises a pair of bridging wires connecting its respective strips of conductor material and providing a shunt connection therebetween, said wires being capable of moving along the entire length of their respective tuning element.
- the strip transmission line circuit of the present invention may be formed directly on the substrate, and placed as close to the device being tested as desired without affecting the performance of either the device or the tuner.
- Another advantage of the present invention' is to provide a tuner which may be connected to the device either through one port to provide an adjustable shunt reactance or through two ports to provide an adjustable two-port reactive network for the device.
- a single port e.g., port 22 of tuning element 10 to the device being tested (not shown)
- element 10 Connecting a single port, e.g., port 22 of tuning element 10 to the device being tested (not shown) enables element 10 to perform as an adjustable single-port shunt reactance, the mobility of bridging wires 16 and 18 accounting for the adjustability of tuning element 10.
- An adjustable two-port reactive network can be obtained by connecting two ports of tuning element 10 to the device being tested. Each of the remaining unconnected ports of tuning element 10 may be open-circuited or short-circuited.
- the open circuit configurations are usually preferable because of the inconvenience of creating a short circuit in a microstrip or stripline medium, and because of the possible requirement of maintaining a bias voltage on the transmission line when active devices are involved.
- Tuners formed in accordance with the present invention in order to match any impedance falling within the Smith chart, comprise two tuning elements as shown generally in Fig. 1 and described hereinabove, arranged in a complementary manner as will be described in greater detail hereinafter in association with Fig. 6, 9, 11 and 14.
- Figs. 2-5 illustrate two alternative known parallel strip circuit arrangements and their equivalent circuits which do not include bridging wires, blocks or sliding contacts.
- Fig. 2 illustrates a parallel-strip circuit 20 similar to tuning element 10 described hereinabove in association with Fig. 1.
- Parallel-strip circuit 20 comprises the conductive strips 12 and 14, and ports 22, 24, 26 and 28 associated with tuning element 10 of Fig. 1, but does not contain bridging wires 16 and 18, since wires 16 and 18 are unnecessary in the development of basic circuit configurations.
- ports 22 and 24 are connected to form terminal 1 which is available for connection to a utilization circuit (not shown), as are ports 26 and 28 connected to form terminal 2 which is also available for connection to a utilization circuit (not shown).
- Fig. 3 illustrates the equivalent circuit 30 associated with parallel-strip circuit 20 of Fig. 2.
- the interconnection of ports 22 and 24 and the interconnection of ports 26 and 28, as described hereinabove in association with Fig. 2 creates transmission line equivalent circuit 30 as shown in Fig. 3.
- the admittance of strip 12 of Fig. 2 is defined as Y 12 and the admittance of strip 14 of Fig. 2 is defined as Y 14 .
- circuit 30, Y 12 +Y 14 is obtained from the application of the well-known 4 X 4 á dmittance matrix of parallel-coupled lines, a detailed derivation of which is contained in the article "Even- and Odd-Mode Waves for Nonsymmetrical Coupled lines in Nonhomogeneous Media” by R. A. Speciale in IEEE Transactions on Microwave Theory and Techniques, Vol. MTT-23, No. 11, November 1975 at pp 897-908.
- the distance ⁇ as shown in Fig. 3, is defined as the electrical length of the equivalent circuit 30.
- ⁇ is defined by the well-known relation where w is the angular frequency of the mode of propagation, I is the physical length of either strip 12 or 14 of parallel-strip circuit 20 of Fig. 2, strips 12 and 14 being of equal length, and v is the velocity of propagation of the mode of propagation.
- Fig. 4 illustrates a parallel-strip circuit 21 which is a variant of parallel-strip circuit 20 of Fig. 2.
- parallel-strip circuit 21 no connection is provided between ports 22 and '24, port 22 forms terminal 1 which is available for connection to a utilization circuit (not shown), and port 24 is open-circuited.
- ports 26 and 28 of parallel-strip circuit 21 are interconnected to form terminal 2.
- Fig. 5 illustrates the equivalent circuit 31 associated with parallel-strip circuit 21 of Fig. 4.
- the impedance of strip 12 of Fig. 4 is defined as Z 12 and the impedance of strip 14 is defined as Z 14 .
- the configuration of strips 12 and 14, in accordance with the present invention yields the following relations: where Y 12 and Y 14 are the admittances as described hereinabove in association with Fig. 3.
- Equivalent circuit 31 comprises a series impedance formed by a short-circuited transmission line of characteristic impedance /(Z 12 +Z 14 ) in cascade with another transmission line of characteristic admittance Y 12 +Y 14 . Both transmission lines have an electrical length ⁇ , which may be obtained by employing equation (1 ).
- Fig. 6 illustrates an exemplary tuner formed in accordance with the present invention comprising two tuning elements 10 1 and 10 2 , each tuning element being as described hereinabove in association with Fig. 1.
- Tuning elements 10, and 10 2 share the conductive strip 14, with the portion designated 14, being the half of strip 14 associated with tuning element 10, and the portion designated 14 2 being the half of strip 14 associated with tuning elements 10 2 .
- Strips 12, and 12 2 are positioned on opposite sides of, and parallel to, strip 14; strip 12, being associated with tuning element 10, and strip 12 2 being associated with tuning element 10 2 .
- Bridging wires 16, and 18, interconnect strips 12, and 14 1 and in a like manner, bridging wires 16 2 and 18 2 interconnect strips 12 2 and 14 2 .
- the electrical lengths ⁇ 1 , ⁇ 1 , ⁇ 2 , ⁇ 2 and ⁇ can be obtained by using equation (1), where the length I of equation (1) is associated with each of the above-mentioned electrical lengths in the following manner: for ⁇ 1 , I is defined as the distance measured between port 22, and bridging wire 16 1 , for ⁇ 1 , I is defined as the distance measured between port 26 1 and bridging wire 18 1 ; for ⁇ 2 , I is defined as the distance measured between port 22 2 and bridging wire 16 2 ; for ⁇ 2 , I is defined as the distance measured between port 26 2 and bridging wire 18 2 ; and for ⁇ is defined as the entire length of either strip 12 1 or 12 2 .
- Each of tuning elements 10 1 and 10 2 is divided into three cascaded sections, tuning element 10 1 comprising cascaded sections 40 1 and 40 2 and 40 3 , and tuning element 10 2 comprising cascaded sections 40 4 , 40 5 and 40 6 .
- Each separate section may be analyzed by comparing the separate sections with parallel-strip circuits 20 and 21 of Figs. 2 and 4, where the port interconnections of parallel-strip circuits 20 and 21 serve to perform in a like manner to bridging wires 16 1 , 18 1 , 16 2 , and 18 2 of the tuner of Fig. 6.
- sections 40 1 and 40 4 can be seen to be similar to parallel-strip circuit 21 of Fig.
- sections 40 2 and 40 5 can be seen to be similar to parallel-strip circuit 20 of Fig. 2 with both ends of sections 40 2 and 40 5 short circuited by wires 16 1 and 18 1 and 16 2 and 18 2 , respectively
- sections 40 3 and 40 6 can be seen to be similar to a mirror image of parallel-strip circuit 21 of Fig. 4 with one end of the sections 40 3 and 40 6 shorted with wires 18 1 and 18 2 , respectively.
- the tuner arrangement of Fig. 6 can be seen to comprise six cascaded sections of parallel-strip circuits in accordance with Figs. 2 and 4.
- the tuner arrangement may, in turn, be analyzed by employing cascaded sections of equivalent circuits 30 and 31 of Figs. 3 and 5, where equivalent circuits 30 and 31 are associated with parallel-strip circuits 20 and 21, respectively. This analysis is described in greater detail hereinafter in association with Fig. 7.
- Fig. 7 illustrates an exemplary all-frequency equivalent circuit associated with the tuner of Fig. 6.
- Fig. 7 comprises cascaded sections of equivalent circuits 30 and 31 of Figs. 3 and 5.
- the overall equivalent circuit is divided into six cascaded sections, each separate section being of the form of equivalent circuit 30 or 31, as denoted by the numeral accompanying each section, and each separate section also being associated with its respective section of Fig. 6, as denoted by the subscript accompanying each numeral.
- section 30 1 of Fig. 7 is of the form of equivalent circuit 30 and is related to the first section, 40 1 , of the tuner of Fig. 6 between ports 22 1 and 24 1 and bridging wire 16 1
- section 31 5 of Fig. 7 is of the form of equivalent circuit 31 and is related to the fifth section, 40 5 , of the tuner of Fig. 6.
- each section of Fig. 7 can be related to the appropriate section of Fig. 6 in the following manner: Z1 2 and Y 1 12 are associated with the portion of strip 12 1 associated with section 40 1 , and are associated with the portion of strip 14 1 associated with section 40 1 , and are associated with the portion of strip 12, associated with section 40 2 , and continuing in a like manner such that Z 6 14 and are associated with section 40 6 of strip 12 2 .
- the arrows shown on the series impedance sections of the equivalent circuit of Fig. 7 are to illustrate the variability of these elements caused by the variations in ⁇ 1 , 8 1 , ⁇ 2 and 8 2 due to the movement of bridging wires 16 1 , 18 1 , 16 2 and 18 2 , respectively.
- the overall lengths of the cascaded transmission line sections ⁇ 1 + ⁇ 1 ,+ ⁇ 1 and ⁇ 2 + ⁇ 2 + ⁇ 2 each of which being equal to ⁇ , do not change, since ⁇ is the electrical length of the entire tuning element, which cannot be varied.
- the specific value of ⁇ is chosen for illustrative purposes only and is not intended to limit the scope and spirit of the present invention.
- the equivalent circuit of Fig. 7 may be reduced to the specific equivalent circuit of Fig. 8.
- the specific circuit comprises four adjustable active elements, L 1 , L 2 , C 1 and C 2 , where each element is defined as follows: where w is the angular frequency, and where each separate element is a function of one of the four electrical lengths ⁇ 1 , ⁇ 1 , ⁇ 2 or ⁇ 2 .
- the equivalent circuit of Fig. 10, therefore, contains only two of the adjustable active elements of the circuit of Fig. 8, C 1 and L 2 , which are functions of the distances ⁇ 1 and ⁇ 2 , respectively. Varying the values of ⁇ 1 and ⁇ 2 from 0 through ⁇ /2 by the movement of bridging wires 18, and 18 2 will cause the tuner associated with Fig. 9 to be capable of matching exactly half of the impedance values falling within the Smith chart.
- Varying the values of ⁇ 1 and ⁇ 2 from 0 through ⁇ /2 by the movement of bridging wires 16 1 and 16 2 will cause the tuner of Fig. 11 to be capable of matching the impedances within the Smith chart not matched by the tuner of Fig. 9.
- Fig. 13 illustrates the Smith chart coverage referred to hereinabove in association with Figs. 10 and 12.
- the darker half of the Smith chart is associated with the tuner of Fig. 9, and the lighter half of the Smith chart is assocaited with the tuner of Fig. 11. Therefore, the combined use of the pair of tuners of Figs. 9 and 11 will be capable of matching any impedance falling within the Smith chart.
- Fig. 14 illustrates another variant of the tuner of Fig. 6.
- bridging wires 16 1 and 18 1 are merged to form a single bridging wire 19 1
- bridging wires 16 2 and 18 2 are merged to form a single bridging wire 19 2
- the distances ⁇ 1 , ⁇ 1 , ⁇ 2 and ⁇ 2 are redefined as follows: ⁇ 1 is defined as the electrical length measured between port 22 1 and bridging wire 19 1 , calculated by using equation (1) where I is the physical length measured between port 22 1 and bridging wire 19 1 .
- ⁇ 2 is defined as the electrical length measured between port 22 2 and bridging wire 19 2 , calculated by using equation (1) where I is the physical length measured between port 22 2 and bridging wire 19 2 .
- the distance ⁇ 1 is defined as the electrical length measured between port 26 1 and bridging wire 19 1 , calculated by using equation (1) where I is the physical length measured between port 26 1 and bridging wire 19 1 .
- the distance ⁇ 2 is defined as the electrical length measured between port 26 2 and bridging wire 19 2 , calculated by using equation (1) where I is defined as the physical length measured between port 26 2 and bridging wire 19 2 .
- the distances, as seen in Fig. 14 are interrelated as follows: The interdependence of ⁇ 1 and ⁇ 1 , and of ⁇ 2 and 8 2 will be discussed in greater detail hereinafter in association with Fig. 15.
- Fig. 15 illustrates the equivalent circuit of the tuner of Fig. 14.
- the four adjustable active elements L 1 , C 1 , L 2 and C 2 are as described hereinabove in association with Fig. 8. In this case, however, the four elements are not independent, rather L, and C 1 are interdependent and L 2 and C 2 are interdependent as shown by the dotted lines in Fig. 15. This interdependence can be determined by referring to Fig. 14, where increasing can be seen to decrease ⁇ 1 . Similarly, increasing ⁇ 2 can be seen to decrease 8 2 . Therefore, the value of L 1 , j(r/Y c )tan ⁇ 1 , varies inversely proportional to C i , jrY c tan ⁇ 1 .
- the value of L 2 , j(r/Y c )tan ⁇ 2 varies inversely proportional to C 2 , jrY c tan ⁇ 2 . Due to this interrelationship, varying the placement of bridging wires 19, and 19 2 will cause the tuner of Fig. 14 to be capable of matching any impedance falling within the Smith chart.
- Figs. 9, 11 and 13 are described as being variants of the embodiment of Fig. 6 and as such are each deemed to include the movable bridging wires 16 1 , 16 2 , 18 1 and 18 2 thereof, even though in Figs. 9 and 11 various ones of the bridging wires are shown in preset positions and even though in Fig. 13 pairs of the bridging wires are merged to form a single bridging wire.
- the structures of Figs. 9, 11 and 13 do not themselves constitute different embodiments of the invention claimed.
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Abstract
Description
- The present invention relates to a strip transmission line tuner circuit comprising a pair of tuning elements disposed over a ground plane, each tuning element comprising a first strip of conductive material and a second strip of conductive material, said second strip being equal in length to and positioned in parallel, spaced apart . relationship with the first strip, the second strip of one of said tuning element being connected in series to the first strip of the other tuning element thereby forming an extended conductive strip having the first strip of the said one tuning element and the second strip of the said other tuning element disposed on opposite sides thereof and in longitudinally spaced relationship thereto. Such a circuit is disclosed in an article "Synthesis of a Class of Strip-Line Filters" by H. Ozaki et al in IRE Transactions on Circuit Theory, Vol. CT-S No. 2, June 1958, at pages 104-109.
- Various microwave devices require the use of adjustable tuners in experimental evaluation of their performance. In the past, microstrip and stripline test fixtures were equipped with transitions to coaxial transmission lines and, therefore coaxial-line multi-slug or multi-stub tuners could be employed. However, the large separation between the device and the tuner limited its use to frequencies less than 10 GHz. There is a need, therefore, for tuners that may be employed directly with the microstrip and stripline medium to overcome the frequency limitation of the coaxial-line tuners.
- One type of tuner that is available for use with microwave transmission lines is disclosed in U.S. Patent 2,757,344. In such known arrangement, a transmission line comprises a wide and a narrow conductor mounted in parallel on opposite sides of a substrate. A tuning element comprises a first and a second conductor disposed in spaced-apart parallel relationship to each other and normal to the narrow conductor of the transmission line. The ends of the tuning element first and second conductors adjacent the narrow line conductor are coupled thereto, and a coupling means is disposed between and in contact with the first and second conductors. The coupling means is longitudinally movable between the first and second adjacent conductors of the tuning element at a distance from the narrow line conductor, and this coupling means forms, in conjunction with the wide conductor of the transmission line directly adjacent the tuning element, and adjustable resonant network.
- The design of stripline filters and directional coupling arrangements are discussed in an article "Coupled-Strip-Transmission-Line Filters and Directional Couplers" by E. M. T. Jones et al in IRE Transactions on Microwave Theory and Techniques, Vol. MTT-4, No. 2, April 1956 at pp. 75-81. There, low-pass, band-pass, all-pass and all-stop basic filter characteristics are obtained from a pair of parallel, spaced-apart, strips either by placing open or short circuits at two of the four available terminals pairs, or by interconnecting two of the terminal pairs. The article further describes how desired performance may be achieved by cascading several of the basic filter sections.
- Another design method for a class of stripline filters is discussed in the aforesaid Ozaki et al article which discloses a method relating to design on an insertion loss basis. Synthesis procedures are presented for the line type, low-pass ladder, high-pass ladder and band-pass ladder filter arrangements. The Ozaki et al arrangements comprise line or ladder cascaded canonical filter sections with each strip section comprising a pair of parallel, spaced-apart, strips having either the same or different widths.
- Although not concerned with microstrip or stripline devices, in U.S. Patent No. 2,247,779, there is disclosed a high frequency transmission line structure which includes a pair of spaced apart tubular conductors having a movable shorting member connected therebetween to effectively adjust the length of the transmission line and thereby adjust the surge impedance of the line.
- The problem remaining in the prior art is to provide a class of tuners which are capable of being formed directly on the microstrip or strip- line medium so as to be close to the device being tested, thereby to increase the usable frequency range of the tuner, and also which are capable of matching any impedance falling within the Smith chart.
- This problem is solved in accordance with the present invention in a strip transmission line circuit as aforesaid by arranging that each tuning element comprises a pair of bridging wires connecting its respective strips of conductor material and providing a shunt connection therebetween, said wires being capable of moving along the entire length of their respective tuning element.
- The strip transmission line circuit of the present invention may be formed directly on the substrate, and placed as close to the device being tested as desired without affecting the performance of either the device or the tuner.
- Another advantage of the present invention'is to provide a tuner which may be connected to the device either through one port to provide an adjustable shunt reactance or through two ports to provide an adjustable two-port reactive network for the device.
- Some exemplary embodiments of the invention will now be described, reference being made to the accompanying drawings, in which:
- Fig. 1 is a view in perspective of an exemplary tuning element containing two bridging wires in accordance with the present invention;
- Figs. 2 and 4 illustrate two known alternative configurations of a parallel-strip circuit for use in analysis of various tuner arrangements formed in accordance with the present invention;
- Figs. 3 and 5 illustrate the equivalent circuits of the known parallel-strip circuits associated with Figs. 2 and 4, respectively, for use in analysis of various tuner arrangements formed in accordance with the present invention;
- Fig. 6 illustrates a complete tuner in accordance with an embodiment of the present invention comprising two of the tuning elements of Fig. 1;
- Fig. 7 illustrates an all-frequency equivalent circuit of the tuner of Fig. 6;
- Fig. 8 illustrates a specific equivalent circuit of the tuner of Fig. 6 for the value of ψ=π/2;
- Fig. 9 illustrates a variant of the tuner of Fig. 6;
- Fig. 10 illustrates a specific equivalent circuit of the tuner of Fig. 9 for the value of ψ=π/2;
- Fig. 11 illustrates another variant of the tuner of Fig. 6;
- Fig. 12 illustrates a specific equivalent circuit of the tuner of Fig. 11 for the value of ψ=π/2;
- Fig. 13 illustrates the Smith chart coverage associated with the tuners of Fig. 9-12;
- Fig. 14 illustrates another variant of the tuner of Fig. 6; and
- Fig. 15 illustrates a specific equivalent circuit of the tuner of Fig. 14 for the value of ψ=π/2.
- Fig. 1 contains an exemplary single parallel-
strip tuning element 10 comprising a pair of adjacent, parallel conductive strips ofequal length ground plane 13, and a pair ofbridging wires strip 12 tostrip 14,bridging wires bridging wire 18 is placed to the right ofbridging wire 16. Tuningelement 10 further comprises fourports strips ports strip 12 andports strip 14. - Connecting a single port, e.g.,
port 22 oftuning element 10 to the device being tested (not shown) enableselement 10 to perform as an adjustable single-port shunt reactance, the mobility ofbridging wires tuning element 10. An adjustable two-port reactive network can be obtained by connecting two ports oftuning element 10 to the device being tested. Each of the remaining unconnected ports oftuning element 10 may be open-circuited or short-circuited. The open circuit configurations are usually preferable because of the inconvenience of creating a short circuit in a microstrip or stripline medium, and because of the possible requirement of maintaining a bias voltage on the transmission line when active devices are involved. - Tuners formed in accordance with the present invention, in order to match any impedance falling within the Smith chart, comprise two tuning elements as shown generally in Fig. 1 and described hereinabove, arranged in a complementary manner as will be described in greater detail hereinafter in association with Fig. 6, 9, 11 and 14. To enable analysis of the tuners formed in accordance with the present invention, Figs. 2-5 illustrate two alternative known parallel strip circuit arrangements and their equivalent circuits which do not include bridging wires, blocks or sliding contacts.
- Fig. 2 illustrates a parallel-
strip circuit 20 similar totuning element 10 described hereinabove in association with Fig. 1. Parallel-strip circuit 20 comprises theconductive strips ports tuning element 10 of Fig. 1, but does not containbridging wires wires circuit 20,ports form terminal 1 which is available for connection to a utilization circuit (not shown), as areports form terminal 2 which is also available for connection to a utilization circuit (not shown). - Fig. 3 illustrates the
equivalent circuit 30 associated with parallel-strip circuit 20 of Fig. 2. In accordance with the well-known transmission line theory, the interconnection ofports ports equivalent circuit 30 as shown in Fig. 3. The admittance ofstrip 12 of Fig. 2 is defined as Y12 and the admittance ofstrip 14 of Fig. 2 is defined as Y14. The admittance ofcircuit 30, Y12+Y14, is obtained from the application of the well-known 4X4ádmittance matrix of parallel-coupled lines, a detailed derivation of which is contained in the article "Even- and Odd-Mode Waves for Nonsymmetrical Coupled lines in Nonhomogeneous Media" by R. A. Speciale in IEEE Transactions on Microwave Theory and Techniques, Vol. MTT-23, No. 11, November 1975 at pp 897-908. The distance ϕ, as shown in Fig. 3, is defined as the electrical length of theequivalent circuit 30. From transmission line theory, ϕ is defined by the well-known relationstrip strip circuit 20 of Fig. 2,strips - Fig. 4 illustrates a parallel-
strip circuit 21 which is a variant of parallel-strip circuit 20 of Fig. 2. In the case of parallel-strip circuit 21, no connection is provided betweenports 22 and '24,port 22forms terminal 1 which is available for connection to a utilization circuit (not shown), andport 24 is open-circuited. Like parallel-strip circuit 20 of Fig. 2,ports strip circuit 21 are interconnected to formterminal 2. - Fig. 5 illustrates the equivalent circuit 31 associated with parallel-
strip circuit 21 of Fig. 4. In accordance with the well-known transmission line theory, the interconnection ofports port 24, as described hereinabove in association with Fig. 4, creates equivalent circuit 31 as shown in Fig. 5. The impedance ofstrip 12 of Fig. 4 is defined as Z12 and the impedance ofstrip 14 is defined as Z14. Further, the configuration ofstrips - Equivalent circuit 31 comprises a series impedance formed by a short-circuited transmission line of characteristic impedance
- Fig. 6 illustrates an exemplary tuner formed in accordance with the present invention comprising two tuning
elements Tuning elements conductive strip 14, with the portion designated 14, being the half ofstrip 14 associated with tuningelement 10, and the portion designated 142 being the half ofstrip 14 associated with tuningelements 102.Strips strip 12, being associated with tuningelement 10, andstrip 122 being associated with tuningelement 102. Bridgingwires wires - The electrical lengths φ1, θ1, φ2, θ2 and ψ can be obtained by using equation (1), where the length I of equation (1) is associated with each of the above-mentioned electrical lengths in the following manner: for φ1, I is defined as the distance measured between
port 22, and bridgingwire 161, for θ1, I is defined as the distance measured betweenport 261 andbridging wire 181; for φ2, I is defined as the distance measured betweenport 222 andbridging wire 162; for θ2, I is defined as the distance measured betweenport 262 andbridging wire 182; and for ψ is defined as the entire length of eitherstrip - Each of tuning
elements element 101 comprising cascaded sections 401 and 402 and 403, and tuningelement 102 comprising cascaded sections 404, 405 and 406. Each separate section may be analyzed by comparing the separate sections with parallel-strip circuits strip circuits wires strip circuit 21 of Fig. 4 with one end of the parallel-strip sections 401 and 404 shorted bywires strip circuit 20 of Fig. 2 with both ends of sections 402 and 405 short circuited bywires strip circuit 21 of Fig. 4 with one end of the sections 403 and 406 shorted withwires - The tuner arrangement may, in turn, be analyzed by employing cascaded sections of
equivalent circuits 30 and 31 of Figs. 3 and 5, whereequivalent circuits 30 and 31 are associated with parallel-strip circuits - Fig. 7 illustrates an exemplary all-frequency equivalent circuit associated with the tuner of Fig. 6. As stated hereinabove in association with Fig. 6, Fig. 7 comprises cascaded sections of
equivalent circuits 30 and 31 of Figs. 3 and 5. Specifically, the overall equivalent circuit is divided into six cascaded sections, each separate section being of the form ofequivalent circuit 30 or 31, as denoted by the numeral accompanying each section, and each separate section also being associated with its respective section of Fig. 6, as denoted by the subscript accompanying each numeral. For example,section 301 of Fig. 7 is of the form ofequivalent circuit 30 and is related to the first section, 401, of the tuner of Fig. 6 betweenports bridging wire 161, and section 315 of Fig. 7 is of the form of equivalent circuit 31 and is related to the fifth section, 405, of the tuner of Fig. 6. - The impedance or admittance of each section of Fig. 7 can be related to the appropriate section of Fig. 6 in the following manner: Z12 and Y1 12 are associated with the portion of
strip 121 associated with section 401,strip 141 associated with section 401,strip 12, associated with section 402, and continuing in a like manner such that Z6 14 andstrip 122. -
- The arrows shown on the series impedance sections of the equivalent circuit of Fig. 7 are to illustrate the variability of these elements caused by the variations in φ1, 81, φ2 and 82 due to the movement of bridging
wires - The variability of the equivalent circuit will be discussed in greater detail hereinafter in association with Fig. 8.
- Fig. 8 illustrates a specific equivalent circuit of the all-frequency equivalent circuit of Fig. 7 depicted for the value of ψ=π/2. The specific value of ψ is chosen for illustrative purposes only and is not intended to limit the scope and spirit of the present invention. Using the value of ψ in association with the relations
strips - It can be shown from well-known basic circuit theory techniques, that independently varying the values of φ1, 81, φ2 and 82 from 0 through π/2 by the movement of bridging
wires - Fig. 9 illustrates a variant of the tuner of Fig. 6 where bridging
wires elements wires - Fig. 10 can be derived from Fig. 8, where in this case jrYctanφ1=jωL1=0 and jrYctanφ2=jωC2=0, since φ1=φ2=0 as shown hereinabove in association with Fig. 9. The equivalent circuit of Fig. 10, therefore, contains only two of the adjustable active elements of the circuit of Fig. 8, C1 and L2, which are functions of the distances θ1 and θ2, respectively. Varying the values of θ1 and θ2 from 0 through π/2 by the movement of bridging
wires - Fig. 11 illustrates another variant of the tuner of Fig. 6 where bridging
wires element wires - Fig. 12 illustrates the equivalent circuit of the tuner of Fig. 11 for the value of ψ=π/2. This equivalent circuit is similar to the circuit of Fig. 8, where in this case jrYctanθ1=jωC1=0 and j(r/ Yc)tanθ2=jωL2=0, since θ1=θ2=0 as shown hereinabove in association with Fig. 11. The equivalent circuit of Fig. 12, therefore, contains only two of the adjustable active elements of the circuit of Fig. 8, L1 and C2, which are functions of φ1 and φ2, respectively. Varying the values of φ1 and φ2 from 0 through π/2 by the movement of bridging
wires - Fig. 13 illustrates the Smith chart coverage referred to hereinabove in association with Figs. 10 and 12. The darker half of the Smith chart is associated with the tuner of Fig. 9, and the lighter half of the Smith chart is assocaited with the tuner of Fig. 11. Therefore, the combined use of the pair of tuners of Figs. 9 and 11 will be capable of matching any impedance falling within the Smith chart.
- Fig. 14 illustrates another variant of the tuner of Fig. 6. In this case, bridging
wires single bridging wire 191, likewise, bridgingwires single bridging wire 192. The distances φ1, θ1, φ2 and θ2 are redefined as follows: φ1 is defined as the electrical length measured betweenport 221 andbridging wire 191, calculated by using equation (1) where I is the physical length measured betweenport 221 andbridging wire 191. In a like manner, φ2 is defined as the electrical length measured betweenport 222 andbridging wire 192, calculated by using equation (1) where I is the physical length measured betweenport 222 andbridging wire 192. The distance θ1 is defined as the electrical length measured betweenport 261 andbridging wire 191, calculated by using equation (1) where I is the physical length measured betweenport 261 andbridging wire 191. Likewise, the distance θ2 is defined as the electrical length measured betweenport 262 andbridging wire 192, calculated by using equation (1) where I is defined as the physical length measured betweenport 262 andbridging wire 192. The distances, as seen in Fig. 14 are interrelated as follows: - Fig. 15 illustrates the equivalent circuit of the tuner of Fig. 14. The four adjustable active elements L1, C1, L2 and C2 are as described hereinabove in association with Fig. 8. In this case, however, the four elements are not independent, rather L, and C1 are interdependent and L2 and C2 are interdependent as shown by the dotted lines in Fig. 15. This interdependence can be determined by referring to Fig. 14, where increasing can be seen to decrease θ1. Similarly, increasing φ2 can be seen to decrease 82. Therefore, the value of L1, j(r/Yc)tanφ1, varies inversely proportional to Ci, jrYctanθ1. Similarly, the value of L2, j(r/Yc)tanθ2, varies inversely proportional to C2, jrYctanφ2. Due to this interrelationship, varying the placement of bridging
wires - It is to be understood that the structures depicted in Figs. 9, 11 and 13 are described as being variants of the embodiment of Fig. 6 and as such are each deemed to include the
movable bridging wires
Claims (1)
- A strip transmission line tuner circuit comprising a pair of tuning elements (101, 102) disposed over a ground plane, each tuning element comprising a first strip of conductive material (121, 142) and a second strip of conductive material (141, 122), said second strip being equal in length to and position in parallel, spaced apart relationship with the first strip, the second strip (141) of one of said tuning elements (10,) being connected in series to the first strip (142) of the other tuning element (102) thereby forming an extended conductive strip (14) having the first strip (12,) of the said one tuning element (101) and the second strip (122) of the said other tuning element (102) disposed on opposite sides thereof and in longitudinally spaced relationship thereto, characterised in that each tuning element (101, 102) comprises a pair of movable bridging wires (161, 181, 162, 182) connecting its respective strips of conductive material and providing shunt connection therebetween, said wires being capable of moving along the entire length (ψ) of their respective tuning element.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US06/083,591 US4267532A (en) | 1979-10-11 | 1979-10-11 | Adjustable microstrip and stripline tuners |
US83591 | 1979-10-11 |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0037413A1 EP0037413A1 (en) | 1981-10-14 |
EP0037413A4 EP0037413A4 (en) | 1982-01-26 |
EP0037413B1 true EP0037413B1 (en) | 1986-04-23 |
Family
ID=22179340
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP80902089A Expired EP0037413B1 (en) | 1979-10-11 | 1981-04-21 | Strip transmission line tuner circuit |
Country Status (6)
Country | Link |
---|---|
US (1) | US4267532A (en) |
EP (1) | EP0037413B1 (en) |
JP (1) | JPS647681B2 (en) |
CA (1) | CA1136300A (en) |
DE (1) | DE3071569D1 (en) |
WO (1) | WO1981001080A1 (en) |
Families Citing this family (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US4475108A (en) * | 1982-08-04 | 1984-10-02 | Allied Corporation | Electronically tunable microstrip antenna |
FR2560442B1 (en) * | 1984-02-24 | 1987-08-07 | Thomson Csf | SLOT LINE SWITCHING AND LIMITING DEVICE, OPERATING IN MICROWAVE |
GB2192494A (en) * | 1986-07-07 | 1988-01-13 | Philips Electronic Associated | Strip transmission line impedance transformation |
US6674293B1 (en) * | 2000-03-01 | 2004-01-06 | Christos Tsironis | Adaptable pre-matched tuner system and method |
USRE45667E1 (en) * | 2000-06-13 | 2015-09-08 | Christos Tsironis | Adaptable pre-matched tuner system and method |
DE10240140A1 (en) * | 2002-08-30 | 2004-03-25 | Siemens Ag | Communication arrangement and transmission unit for transmitting information via at least one transmission line and a circuit arrangement connectable to the transmission unit |
CN113109692B (en) * | 2021-03-31 | 2023-03-24 | 中国电子科技集团公司第十三研究所 | Microstrip circuit debugging method and adjusting module |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
NL30417C (en) * | 1928-03-23 | |||
US2247779A (en) * | 1940-06-01 | 1941-07-01 | Gen Electric | High frequency apparatus |
US2757344A (en) * | 1953-01-12 | 1956-07-31 | Itt | Tuner |
US3796976A (en) * | 1971-07-16 | 1974-03-12 | Westinghouse Electric Corp | Microwave stripling circuits with selectively bondable micro-sized switches for in-situ tuning and impedance matching |
CA1097755A (en) * | 1976-02-26 | 1981-03-17 | Mitsuo Makimoto | Electrical tuning circuit |
US4096453A (en) * | 1977-05-19 | 1978-06-20 | Gte Automatic Electric Laboratories Incorporated | Double-mode tuned microwave oscillator |
-
1979
- 1979-10-11 US US06/083,591 patent/US4267532A/en not_active Expired - Lifetime
-
1980
- 1980-09-25 JP JP55502548A patent/JPS647681B2/ja not_active Expired
- 1980-09-25 DE DE8080902089T patent/DE3071569D1/en not_active Expired
- 1980-09-25 WO PCT/US1980/001246 patent/WO1981001080A1/en active IP Right Grant
- 1980-10-02 CA CA000361367A patent/CA1136300A/en not_active Expired
-
1981
- 1981-04-21 EP EP80902089A patent/EP0037413B1/en not_active Expired
Non-Patent Citations (5)
Title |
---|
"Synthesis of a class of strip line filters", Ozakietal, IRE transactions on circuit theory, vol. CT-5 No 2, June 1958 * |
"Techniques de l'Ingénieur", pages 9-12, E 647, 6. June 1974 * |
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, vol. MTT-28, no. 7, July 1980, pages 725-732 New York, U.S.A., A.A.M. Saleh: "Transmission-line identities for a class of interconnected coupled-line sections with application to adjustable microstrip and stripline tuners" * |
IRE transactions on microwave theory and techniques, vol. MTT-4, No2 April 1956: "Coupled-Strip-Transmission-Line Filters and Directional Couplers", E.M.T. Jones et al. * |
The new penguin dictionary of electronics, page 314, Penguin Books 1979 * |
Also Published As
Publication number | Publication date |
---|---|
JPS647681B2 (en) | 1989-02-09 |
CA1136300A (en) | 1982-11-23 |
EP0037413A4 (en) | 1982-01-26 |
EP0037413A1 (en) | 1981-10-14 |
DE3071569D1 (en) | 1986-05-28 |
US4267532A (en) | 1981-05-12 |
JPS56501346A (en) | 1981-09-17 |
WO1981001080A1 (en) | 1981-04-16 |
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